Competition between superconductivity and antiferromagnetic glass freezing in the pseudogap regime of La<sub>1.8-x</sub>Eu<sub>0.2</sub>Sr<sub>x</sub>CuO<sub>4</sub>
ORAL
Abstract
A. Missiaen, H. Mayaffre, D. LeBoeuf, M.-H. Julien, Laboratoire des Champs Magnétiques Intenses, Grenoble, France
S. Pyon, Department of Applied Physics, University of Tokyo, Japan
T. Takayama and H. Takagi, Max Planck Institute for Solid State Research, Stuttgart, Germany
A recent NMR and ultrasound study of the cuprate superconductor La2-xSrxCuO4 [Frachet et al. Nat. Phys. 16, 1064 (2020)] revealed that p* ~ 0.19, the critical hole doping for the pseudogap phase at T = 0, coincides with a quantum phase transition from frozen to fluctuating antiferromagnetism, once superconductivity has been quenched in high magnetic fields. Here, we present 139La nuclear magnetic resonance (NMR) measurements of the temperature, magnetic field and hole-doping dependence of spin fluctuations in the sister compound La1.8-xEu0.2SrxCuO4. We find similar field-dependent glassy freezing as in La2-xSrxCuO4, up to a doping ~ 0.24, consistent with p* for La1.8-xEu0.2SrxCuO4. That the specific heat (measured in high magnetic fields) is sharply enhanced around the same doping in this material [Michon et al., Nature 567, 218 (2019)], suggests that the two observations are connected, one way or another.
S. Pyon, Department of Applied Physics, University of Tokyo, Japan
T. Takayama and H. Takagi, Max Planck Institute for Solid State Research, Stuttgart, Germany
A recent NMR and ultrasound study of the cuprate superconductor La2-xSrxCuO4 [Frachet et al. Nat. Phys. 16, 1064 (2020)] revealed that p* ~ 0.19, the critical hole doping for the pseudogap phase at T = 0, coincides with a quantum phase transition from frozen to fluctuating antiferromagnetism, once superconductivity has been quenched in high magnetic fields. Here, we present 139La nuclear magnetic resonance (NMR) measurements of the temperature, magnetic field and hole-doping dependence of spin fluctuations in the sister compound La1.8-xEu0.2SrxCuO4. We find similar field-dependent glassy freezing as in La2-xSrxCuO4, up to a doping ~ 0.24, consistent with p* for La1.8-xEu0.2SrxCuO4. That the specific heat (measured in high magnetic fields) is sharply enhanced around the same doping in this material [Michon et al., Nature 567, 218 (2019)], suggests that the two observations are connected, one way or another.
–
Presenters
-
Anne Missiaen
CNRS/GHMFL
Authors
-
Anne Missiaen
CNRS/GHMFL
-
Marc-Henri Julien
CNRS/GHMFL, Laboratoire National des Champs Magnetiques Intenses
-
David LeBoeuf
CNRS/GHMFL, Laboratoire National des Champs Magnetiques Intenses
-
Hadrien Mayaffre
CNRS/GHMFL, Laboratoire National des Champs Magnetiques Intenses
-
Sunseng Pyon
University of Tokyo (Japan), University of Tokyo
-
Tomohiro Takayama
University of Tokyo (Japan), Max Planck Institute for Solid State Research
-
Hidenori Takagi
University of Tokyo (Japan), Max Planck Institute for Solid State Research, Max Planck Institute for Solid State Research, Stuttgart, Germany